Microquasars
If you want to use this webpage please do so, however
remember to acknowledge it:
Chaty S., www.aim.univ-paris7.fr/CHATY
This work was made by Sebastien Delautier (Supelec student, engineering school) during a one month internship at the CEA/Irfu under the direction of Sylvain Chaty. A similar work was also made for a few dust enshrouded INTEGRAL sources.
Name | RA | DE | Binary characteristics | Jet | X rays | INTEGRAL gamma flux (mW/m2) | IR (2Mass Catalogue) | IR (Litterature) | UV | Radio | Optical | Notes | ||||||||||||||||||||||||||||||||||||||||
J2000 | J2000 | Compact Object | Companion star | Binary type | Magnitude | Inclination | Speed | Average flux | F3 | F10 | F30 | F60 | Average Mag | Average | UV obs | Average | Range | Average flux at 1,4Ghz (mJy) | Average flux at other frequencies (litt) | Average | Band | |||||||||||||||||||||||||||||||
h m s | h m s | Type | Mass (Msun) | Porb (d or hr) | Spectral type | Mass(Msun) | Mass Ratio | Type | (V band) | (deg) | (microJy, 2-12keV) | 3-10keV | 10-30keV | 20-60keV | 60-200keV | J | H | K | mag (K band) | flux | (NVSS catalogue) | Flux | Freq | Mag | ||||||||||||||||||||||||||||
Microquasars | ||||||||||||||||||||||||||||||||||||||||||||||||||||
LS I +61°303 | 02 36 | +61 0 | ? | 1 | 26,4960+-0,0028d | B0 Ve star | 10-15 | HMXB | 10,8 | 30+-20 | 0,6c | 2,65E-11 | 4,51E-12 | 4,30E-13 | 7,21E-17 | 8,621+-0,024 | 8,228+-0,021 | 7,917+-0,023 | X | 42,2+-1,3 | 1-17E31 erg/s | |||||||||||||||||||||||||||||||
CI Cam | 04 21 | +56 0 | White dwarf? | 19,41+-0,02d | B2 IIIe/B[e] | HMXB | 11,86 | 0,15c | 2000 | 3,48E-08 | 5,68E-08 | 3,70E-08 | 2,77E-09 | 13,594+-0,086 | 11,439 | 10,228 | X ray outbursts | |||||||||||||||||||||||||||||||||||
XTEJ1118+480 | 11 18 | +48 0 | Black hole | 6,1+-0,3 | 4,1hr | 0,037+-0,008 | LMXB | 12,25 | 71-82 | 0,4c | 40 | 5,36E-09 | 1,11E-09 | 1,19E-10 | 2,42E-14 | 12,76+-0,023 | 12,444+-0,030 | 12,084+-0,02 | X | 8,68+-0,87mJy | 15,2Ghz | I=12,68+-0,05 | V | UV var. lags behind X-rays by 1-2 s | ||||||||||||||||||||||||||||
XTEJ1550-564 | 15 50 | -56 4 | Black hole? | 10,7 | 36,96hr | G/K subgiant | LMXB | 16,6-21,4 | 73,1 | 0,55c down to 0,16c | 600-7000 | 1,38E-10 | 2,85E-11 | 3,05E-12 | 6,23E-16 | ? | ? | ? | 10+-2,5mJy | 4,8-8,6Ghz | 17 | V | strong aperiodic X-ray variability | |||||||||||||||||||||||||||||
4U1630-47 | 16 34 |
-47 26 | LMXB | 60-75 | <2-1400 | 4,10E-10 | 8,49E-11 | 9,08E-12 | 1,85E-15 | 13,65+-0,05 | ||||||||||||||||||||||||||||||||||||||||||
GRO J1655-40/ V* V1033 Sco | 16 55 | -40 | Black hole | 7 | 2,6219+-0,0002d | 2,3 | LMXB | 14,2-17,3 | 70,2+-1,9 | 0,27+-0,03c | 1600 | 1,46E-10 | 3,28E-11 | 6,09E-12 | 1,88E-12 | 13,516+-0,029 | 12,997+-0,044 | 12,744+-0,034 | 12,06-13,4 | X | 18,1-18,9 | 216-286nm | 15,1-16,3 | V | repeated X-ray outbursts; superluminal jets; X-ray dips;reprocession of X-ray into opt. and UV emissi | |||||||||||||||||||||||||||
GX339-4 | 17 02 | -48 | Black hole | 0,61916+-0,00065d | LMXB | 15,5 | 1,5-900 | 4,41E-12 | 7,41E-12 | 1,05E-11 | 2,05E-11 | 15,911+-0,137 | 15,404+-0,150 | 14,973+-0,138 | ||||||||||||||||||||||||||||||||||||||
KS1731-260 | 17 31 | -26 0 | Neutron star | 1,4 | 1-3d | LMXB | <10-110 | ? | ? | ? | ? | 14,833+-0,061 | 13,548+-0,070 | 13,024+-0,052 | 18,5-19 | 156,3+-5,5 | X-ray bursts | |||||||||||||||||||||||||||||||||||
1E 1740,7-2942 | 17 40 70 | -29 42 | ? | 10 | 12,73d | red giant? | LMXB | 80 | 0,7c | 4-30 | 2,44E-08 | 3,88E-08 | 4,08E-08 | 2,97E-08 | ? | ? | ? | repeated outbursts of hard emission; double-sided radio jet | ||||||||||||||||||||||||||||||||||
XTE J1748-2829 | 17 48 | -28 8 | ? | LMXB | 640 | 9,29E-12 | 2,74E-12 | 3,03E-13 | 6,22E-17 | 16,478+-0,115 | 16,274 | 14,771 | radio jets | |||||||||||||||||||||||||||||||||||||||
GRS1758-258 | 17 58 | -25 8 | ? | 8-9 | 18,45+-0,03d | K0 III giant | 10 | LMXB | <=0,3 | 1250 | 0,14+-0,01/30,3+-1 | 4,8/8,6Ghz | no X-ray pulsations;long and short term X-ray vars | |||||||||||||||||||||||||||||||||||||||
V4641 Sagitarii | 18 19 30 | -16 25 25 | Black hole | 9,61+2,08-0,88 | 2,81678+-0,00056d | late B star/B9III | 6,53 +1,6/-1,03 | 0,666+-0,076 | LMXB | 8,8-13,5 | 60-70,7 | 0,9c | 1-13000 | 4,10E-11 | 8,48E-12 | 9,07E-13 | 1,85E-16 | 12,532+-0,032 | 12,364+-0,028 | 12,270+-0,032 | 13,1+-0,6 | |||||||||||||||||||||||||||||||
V691 CrA | 18 22 | -37 1 | Neutron star | 1,4 | 5,57hr | 0,40-0,43 | LMXB | 15,3-16,3 | 81-84 | 10-25 | 1,68E-09 | 7,25E-10 | 2,06E-10 | 2,01E-12 | 15,285+-0,054 | 15,297+-0,105 | 15,450+-0,194 | X | accretion disc corona | |||||||||||||||||||||||||||||||||
LS 5039 | 18 26 20 | -14 50 | Neutron star | 1,4 | 4,117+-0,011d | O7V | 10-40 | HMXB | 11,23 | 30 | >0,15c | 0,3 | 5,22E-12 | 8,51E-12 | 5,55E-12 | 4,15E-13 | 9,024+-0,026 | 8,751+-0,022 | 8,604+-0,022 | 23,4+-0,9 | bipolar jets | |||||||||||||||||||||||||||||||
XTE J1859+226/V406 Vul | 18 59 | 22 6 | Black hole | 5-12 | 9,16+-0,08hr | 0,68-1,12 | LMXB | 15,31-15,75 | 60? | ? | 600 | 8,63E-09 | 1,79E-09 | 1,91E-10 | 2,90E-14 | ? | ? | ? | 13,833-16,67 | X | ||||||||||||||||||||||||||||||||
SS433 | 19 09 | +04 8 | 30 | 13,082d | A5-A7I | 9 | HMXB | 14,2 | 78,8 | 0,26c | 2-10 | 6,52E-09 | 2,81E-09 | 7,97E-10 | 7,80E-12 | 9,398+-0,021 | 8,739+-0,029 | 8,163+-0,024 | 879,4+-26,4 | accretion disk; high speed jets; extended X-ray lobes | ||||||||||||||||||||||||||||||||
GRS1915+105 | 19 15 | +10 5 | Blackhole | 14+-4 | 33,5d | K-M III | 1,2+-0,2 | LMXB | I=23.4 | 70+-2 | 0,60c | 300 | 1,46E-10 | 3,28E-11 | 6,09E-12 | 1,88E-12 | 15,549+-0,063 | 13,416+-0,031 | 12,415+-0,035 | 12,95+-0,14 | 160mJy | 8,4Ghz | quasi periodic in IR, radio and mm band; repeated relativistic ejections;IR synchrotron emissions | |||||||||||||||||||||||||||||
Cygnus X-1 | 19 58 21,7 | +35 12 | Blackhole | 13,5-29 | 5,6d | 29-50 | HMXB | 8,90 | 28-38 | ? | 1,67E-08 | 2,15E-08 | 2,52E-08 | 2,89E-08 | 6,872+-0,023 | 6,562+-0,18 | 6,501+-0,020 | |||||||||||||||||||||||||||||||||||
Cygnus X-3 (V1521) | 20 30 | +40 7 | ? | 1,4-3 | 4,8hr | 6-10 | HMXB | I=20,0 | 70 | 0,48-0,81c | 90-430 | 6,83E-10 | 9,14E-10 | 1,13E-09 | 1,75E-09 | 15,309+-0,059 | 13,192+-0,057 | 11,921+-0,031 | 16,3 | 87,3+-3,2 | 100mJy | cm | 21,3 | I | radio jets and lobes; radio outbursts; No X ray pulsations | |||||||||||||||||||||||||||
XTE J1720-318 |
17 19 59 |
-31 44 59 |
Blackhole |
HMXB |
0.27+-0.06 |
8.5 |
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Sco X-1 |
16 19 55 |
-15 38 25 |
LMXB |
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Statistics | ||||||||||||||||||||||||||||||||||||||||||||||||||||
mean | 5,86E-09 | 7,33E-09 | 6,21E-09 | 4,61E-08 | 12,834 | 12,047 | 11,505 | |||||||||||||||||||||||||||||||||||||||||||||
rms | 1,02E-08 | 1,64E-08 | 1,37E-08 | 1,74E-07 | 3,126 | 2,950 | 2,817 | |||||||||||||||||||||||||||||||||||||||||||||
median | 4,1E-10 | 8,49E-11 | 6,25E-11 | 1,88E-12 | 13,555 | 12,720 | 12,177 | |||||||||||||||||||||||||||||||||||||||||||||
Explanations |
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Introduction |
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About the compact object |
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About the binary type |
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Multi wavelength
characteristics |
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Radio data |
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Gamma, IR and radio |
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Statistics |
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Microquasars are smaller cousins of quasars.
They are named after quasars, as they have some common characteristics:
strong and variable radio emission often seen as radio jets, and a
binary system with a black hole or white dwarf as the compact object
and a companion star. |
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In quasars, the black hole is
supermassive (millions of solar masses), while in microquasars the
black hole mass is a few solar masses. In microquasars, the accreted
mass comes from the companion star and the accretion disk is very
luminous in X-rays. |
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Microquasars are sometimes called 'radio-jet
X-ray binaries' to distinguish them from other X-ray binaries. Most of
the radio emission comes from relativistic jets, often showing apparent
superluminal motion. |
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Microquasars are very
important for the study of relativistic jets. The jets are formed close
to the black hole, and timescales near the black hole are proportional
to the mass of the black hole. Therefore, ordinary quasars take
centuries to go through variations a microquasar experiences in one day. |
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About this chart |
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The first step was to build a list of known
microquasars. I used the Astrophysics Data System (ADS) with the
keyword microquasar and I read the articles in order to establish the
first column of the chart with accuracy. The
list is ordered by Right Ascension going up. |
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The chart is based on
literature and observation catalogues. The first half gathering the
binary characteristics (type, mass, period, jet speed) relies on
articles found about the source. It is important to notice that the V
magnitude comes from articles in this part of the chart, not from
catalogues. |
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About the compact object |
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The type of compact object is based on
literature and is linked with the jets speed. This is why I gathered
the available speeds in a dedicated column. Actually the 0.5c speed
limit seems to be a frontier for the nature of the compact object:
neutron star under 0.5c and black hole above. The jet speed of
J1550-564 is particular: a deceleration of the jet was observed, from
0,55c to 0,16c (because of the interaction with the interstellar
medium). |
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About the binary type |
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I was not able to find all the
mass values of the companion star. Consequently the type Low Mass X ray
Binary and High Mass X ray Binary is mostly taken from |
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Q.Z.Liu et al., A catalogue of low-mass X-ray
binaries, Astronomy & Astrophysics 368, 1021-1054 (2001) |
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Q.Z.Liu et al., A
catalogue of high-mass X-ray binaries, Astronomy & Astrophysics,
Suppl series 147,25-49 (2000) |
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The mass ratio is equal to Mcompanion/Mcompact object | ||||||||||||||||||||||||||||||||||||||||||||||||||||
Multi wavelength
characteristics |
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The X ray average fluxes in
the 2-12keV band are taken from the catalogues established by Q.Z. Liu
et al. |
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The first V magnitude column is also taken from
Q.Z. Liu et al |
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The optical (second optical column, at the end
of the chart) and UV values come from articles. Concerning UV, the
cross indicates the observational evidence of a UV counterpart but I
was not able to find the related values. |
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Radio data |
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The radio data is half from the literature, with
various frequencies and half from the NVSS catalogue, with a frequency
of 1.4GHz (see the text below for further information) |
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Gamma, IR and radio |
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After a search with Simbad for
the current coordinates of the object, I used Vizier within the
catalogue of INTEGRAL sources. Then I plotted the result with Aladdin
and added the Simbad analysis of the area to make sure I had the good
source. I also added X ray, IR and radio
data. Hence an accurate selection of the sources in IR and radio could
be made. However in some cases, radio and X-ray data
do not accurately help to definite the position of the IR counterpart.
Therefore I selected only the nearest (from the Simbad reference)
infrared source. |
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Statistics |
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As I was able to find comprehensive data in IR
and Gamma for the 17 microquasars, I calculated mean, rms and median.
The gamma-ray values can vary with a factor 100 to 1000 so you should
only consider the median. |
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This work has two goals.
First, it gathers available data about the microquasars in a unique
chart, making it easier to read. Secondly, it can help to determine the
typical characteristics of the microquasars (radio jets, x-ray and
gamma-ray emissions). The statistics were calculated in order to
compare the fluxes of new INTEGRAL sources with the flux of the
microquasars and help to draw conclusions on the nature of the source. |
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